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Master Equation - Based Numerical Simulation in a Single Electron ...

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244<br />

<strong>Numerical</strong> <strong>Simulation</strong>s of Physical and Eng<strong>in</strong>eer<strong>in</strong>g Processes<br />

<br />

Change of charge <strong>in</strong> capacitor is = − . Consider the equation (6b) <br />

becomes,<br />

<br />

= − ,<br />

= ,<br />

= e<br />

(14)<br />

<br />

Change of charge <strong>in</strong> capacitor is = − . Consider the equation (6c) <br />

becomes,<br />

<br />

= − − − ,<br />

=− ,<br />

=− e<br />

(15)<br />

2. Work done when one electron tunnel through capacitor ( ⟶ +)<br />

Work done by power supply is a sum of multiplication between charge change <strong>in</strong> each<br />

term<strong>in</strong>al and a given power supply voltage. Thus, when one electron tunnel through the<br />

capacitor , the work becomes,<br />

( ) = (+ ) +( ) + ( ) ×0,<br />

( ) = + <br />

<br />

− <br />

<br />

<br />

<br />

The same calculation can be done when the s<strong>in</strong>gle electron tunnel through the capacitor ,<br />

as shown <strong>in</strong> Figure 3.<br />

Fig. 3. The charge flow <strong>in</strong> the s<strong>in</strong>gle electron transistor circuit when an electron tunnels<br />

through the capacitor . 1. Change <strong>in</strong> charge when an electron through the capacitor ( ⟶ +)<br />

Change of potential <strong>in</strong> the dot due to electron tunnel<strong>in</strong>g ( ⟶− or ⟶−1) is<br />

<br />

= − , thus :<br />

(16)

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